Superconducting magnet, particularly for MRI imaging apparati and method of using same

ABSTRACT

A superconducting magnet, in which a static magnetic filed is generated in a region of interest, i.e. a predetermined volume in which the part under examination has to be placed for imaging characterised in that it is provided with means for generating a uniform annular distribution of electric currents enclosing the polyhedral cavity.

CROSS-REFERENCE TO RELATED APPLICATIONS

[0001] The present application claims the priority of Italian Patent Application No. IT SV2001A0000034, filed on Oct. 2, 2001, the entire contents of which is hereby incorporated herein by reference.

BACKGROUND OF THE INVENTION

[0002] 1. Field of the Invention

[0003] The invention relates to a superconducting magnet, in which a static magnetic filed is generated in a region of interest, i.e. a predetermined volume in which the part under examination has to be placed for imaging.

[0004] The invention deals with magnets having a closed current distribution as well as magnets having an open current distribution which are derived from the closed ones.

[0005] 2. Discussion of Related Art

[0006] Real time NMR imaging in a surgical procedure requires open magnets that facilitate access to the surgical area by the surgeon and the surgical instrumentation. Furthermore, a magnet must be designed for a field high enough to achieve an image reconstruction within acceptable time intervals. Such a requirement results in rather larger magnetic structures, particularly in the case of permanent magnets. For high fields, well above 1 Tesla, a magnet design cannot make use of ferromagnetic materials that saturate above 1.5 Tesla, and a design based on permanent magnets with remanences below 1.5 Tesla becomes very inefficient. As a consequence, very high fields are the domain of superconducting magnets and low to medium fields up to a 0.5 Tesla range are now the undisputed domain of permanent magnets.

[0007] In the 1 Tesla range, superconducting and permanent magnet technologies can both be used to provide for efficiently generating the magnetic field having the desired strength and homogeneity.

[0008] Furthermore both technologies may be combined in designs that take full advantage of both technologies resulting in powerful and efficient new structures.

OBJECTS AND SUMMARY

[0009] Accordingly, it is an object of the present invention to provide for a closed magnet structure using the superconducting magnet technique in order to generate magnetic fields with a magnitude about 1 Tesla and reducing at the same time the dimensions and weight of the magnetic structure.

[0010] Another object of the present invention is to provide for an open magnet structure using the superconducting magnet technique in order to generate magnetic fields with a magnitude about 1 Tesla and reducing at the same time the dimensions and weight of the magnetic structure.

[0011] It is a further object of the present invention to provide an open superconducting magnet having high order harmonic correction means of the field distortions of different harmonic order in the region of the opening.

[0012] One embodiment of the invention achieves its first aim by providing a closed superconducting magnet with means for generating a uniform annular distribution of electric currents enclosing the polyhedral cavity. Furthermore the distribution of electric currents is composed of uniform surface currents on interfaces towards the enclosed cavity; on opposed plane peripheral boundaries surfaces and in which the current density at each peripheral boundary surface is defined by

{right arrow over (j_(1,h))}=−{right arrow over (η)}×{right arrow over (H)} _(h)

[0013] where {right arrow over (η)} is a unity vector perpendicular to the corresponding peripheral plane boundary and {right arrow over (H)}_(h) is the intensity vector associated with the region enclosed by said plane boundary.

[0014] According to a further embodiment, the structure of currents may be divided into different regions each one having a correspondent interface to the polyhedral cavity and a correspondent peripheral boundary surface towards the external medium and each one having an adjacent region and a common plane interface to that adjacent region.

[0015] In this case, the current at the peripheral boundary of each region being defined by

{right arrow over (j_(1,h))}=− {right arrow over (η)}×{right arrow over (H)} _(h)

[0016] where {right arrow over (η)} is a unity vector perpendicular to the external plane boundary of the h-region and oriented outwards with reference to the centre of the cavity; and {right arrow over (H)}_(h) is the field intensity at the h-region or at the h-field generating element.

[0017] A uniform field solution exists for any combination of intensity vectors Hh, Hh+1 of the different regions of the current structure, for which the tips of the intensity vectors lay on ideal lines parallel to the corresponding interfaces to the cavity, the origin being defined by the common intersection axis of two adjacent or subsequent interfaces of adjacent or subsequent regions of the opened annular structure of currents.

[0018] The orientation of the difference vector of the magnetic intensity vectors of two adjacent or subsequent regions defines the orientation of the common plane interface between two subsequent or adjacent regions.

[0019] The magnitude of the difference vector defines the current density at the plane common interface between the regions.

[0020] The peripheral plane boundaries of each region is parallel to the intensity vector of the field generated in the said region or by the same field generating element.

[0021] The current density on each interface may, be generated by independent sources corresponding to the different regions. Thus the closed superconducting magnet is formed by several coils, the windings of which enclose polyhedral volumes having shapes corresponding to the geometrical shape of the different regions in which the structure of current is divided extending over the surfaces of the said volumes.

[0022] In this case, the current density on each face of the winding is defined by:

{right arrow over (j)} _(h,k) =−{right arrow over (η)} _(h,k) ×{right arrow over (H)} _(h)

[0023] where index h defines the different volumes of the different regions and k the different faces of the ideal geometric figure defining the said volume.

[0024] Further improvements or embodiments are described with more detail in the following detailed description of the preferred embodiments.

[0025] An open magnet structure according to a preferred embodiment of the present invention includes means for generating a uniform annular distribution of electric currents enclosing the polyhedral cavity.

[0026] The distribution of currents is defined according to a correspondent closed distribution of currents which is opened at the relevant region for carrying out imaging.

[0027] Similarly to the closed magnet structure according to the embodiments disclosed above, also in the case of the open superconducting magnet the distribution of electric currents is composed of uniform surface currents on interfaces towards the enclosed cavity; on opposed plane peripheral boundaries surfaces; and in which the current density at each peripheral boundary surface is defined by

{right arrow over (j_(1,h))} =−{right arrow over (η)}×{right arrow over (H)} _(h)

[0028] where {right arrow over (H)}_(h) is a unity vector perpendicular to the corresponding peripheral plane boundary and Hh is the intensity vector associated with the region enclosed by said plane boundary.

[0029] Also in the case of the open magnet structure, the structure of currents may be divided into different regions each one having a correspondent interface to the polyhedral cavity and a correspondent peripheral boundary surface towards the external medium and each one having an adjacent region and a common plane interface to that adjacent region, except at the relevant which correspond to one of the said region in which the structure of currents is divided and at which the opening of the structure is provided where the said common plane interfaces of the end regions forms the two opposite surfaces delimiting the relevant region.

[0030] In this case, the current at the peripheral boundary of each region being defined by

{right arrow over (j_(1,h))} =−{right arrow over (η)}×{right arrow over (H)}_(h)

[0031] where {right arrow over (η)} is a unity vector perpendicular to the external plane boundary of the h-region and oriented outwards with reference to the centre of the cavity; {right arrow over (H)}_(h) is the field intensity at the h-region or at the h-field generating element.

[0032] A uniform field solution exists for any combination of intensity vectors Hh, Hh+1 of the different regions of the current structure, for which the tips of the intensity vectors lay on ideal lines parallel to the corresponding interfaces to the cavity, the origin being defined by the common intersection axis of two adjacent or subsequent interfaces of adjacent or subsequent regions of the opened annular structure of currents.

[0033] The orientation of the difference vector of the magnetic intensity vectors of two adjacent or subsequent regions defines the orientation of the common plane interface between two subsequent or adjacent regions.

[0034] The magnitude of the difference vector defines the current density at the plane common interface between the regions.

[0035] The peripheral plane boundaries of each region is parallel to the intensity vector of the field generated in the said region or by the same field generating element.

[0036] The current density on each interface may be generated by independent sources corresponding to the different regions. Thus the open superconducting magnet is formed by several coils, the windings of which enclose polyhedral volumes having shapes corresponding to the geometrical shapes of the different regions in which the structure of current is divided extending over the surfaces of the said volumes.

[0037] In this case, the current density on each face of the winding is defined by:

{right arrow over (j)} _(h,k)=−{right arrow over (η)}_(h,k) ×{right arrow over (H)} _(h)

[0038] where index h defines the different volumes of the different regions and k the different faces of the ideal geometric figure defining the said volume.

[0039] Further improvements or embodiments are described with more detail in the following detailed description of the preferred embodiment.

[0040] According to a further embodiment, an open superconducting magnet is constructed according to a hybrid design approach. In this embodiment, the structure combines superconducting windings and permanent magnets as well as ferromagnetic materials.

[0041] Some rare-earth magnetic alloys exhibit high intrinsic coercivity, and cannot be demagnetized in strong fields far above 1 Tesla. As a consequence, both ferromagnetic materials and high intrinsic coercivity permanent magnets can be used to generate the desired field configuration in the region of interest at field levels exceeding 1 Tesla. Conversely, the total flux of the induction can be effectively generated and channeled in the superconducting windings where large electric currents make it possible to minimize the magnet dimensions.

[0042] The above mentioned embodiment includes providing a filter structure for compensating the low order harmonic magnetic field distortion at the relevant region where imaging is to be carried out by providing at the opposed and spaced apart interface surfaces defining the opening of the cavity plates of ferromagnetic materials and/or permanent magnets.

[0043] The relevant theory and the particular construction is disclosed in the following detailed description of the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

[0044]FIG. 1 is a schematic view of a structure of uniform surface current densities at two adjacent regions of a closed current structure.

[0045]FIG. 2 is a schematic view of a current structure according to the present invention for field confinement within peripheral boundaries at two adjacent regions, i.e., field generating elements.

[0046]FIG. 3 shows a field generating element formed by an independent winding with uniform surface current densities.

[0047]FIG. 4 shows a perspective view of a closed current structure from which also the open structure according to an embodiment of the present invention is derived.

[0048]FIG. 5 shows a schematic side view of the structure according to FIG. 4.

[0049]FIG. 6 shows the independent windings of the closed current structure according to FIGS. 4 and 5.

[0050]FIG. 7 show the insertion of a plate having infinite permeability perpendicular to the axis of the field of the relevant region, i.e., the region where imaging is performed.

[0051]FIG. 8 shows the region of the opening of the superconducting magnet according to an embodiment of the invention with two pole plates.

[0052]FIG. 9 shows the equipotential lines between two plates

[0053]FIG. 10 shows an equivalent current loop component of the filter structure formed by ferromagnetic plates.

[0054]FIG. 11 is a schematic cross section of the open superconducting magnet with filters according to an embodiment of the invention.

[0055]FIG. 12 is a diagram of the superconducting shunt.

[0056]FIG. 13 shows the arrangement of the conductors at the interfaces between adjacent windings of adjacent field generating elements.

[0057]FIG. 14 shows the lines of flow of the current density in one element of the filter structure.

[0058]FIG. 15 shows an example of closed lines of the current density in one element of the filter structure.

[0059]FIG. 16 shows the radial lines of flux

[0060]FIG. 17 show a circular coil.

[0061]FIG. 18 show the dipole moment density generated by the circular coil according to FIG. 17.

DETAILED DESCRIPTION OF THE REFERRED EMBODIMENTS

[0062]FIG. 1 shows a schematic view of a structure of uniform surface current densities at two adjacent regions of a closed current structure.

[0063] A uniform field {right arrow over (H)}_(o) can be generated in an arbitrarily assigned closed polyhedral cavity by enclosing the cavity either in a structure of a uniformly magnetized polyhedron or a structure of electric currents. A self-shielding distribution of electric currents is composed of uniform surface currents on plane surfaces, as indicated in the schematic of FIG., 1, where surface current densities {right arrow over (j)}_(h), {right arrow over (j)}_(h+1) flow on interfaces S_(h), S_(h+1) that are part of the boundary of the polyhedral cavity. The uniform field {right arrow over (H)}₀ and the plane interfaces S_(h), S_(h+1) postulate uniform intensities in the two regions that interface with the cavity, and, as a consequence, the two regions must have a common plane interface V_(h) as indicated in FIG. 1, where a uniform current density flows to satisfy the boundary conditions. The condition of existence of a uniform field solution in a structure of electric currents is equivalent to the condition of existence of a uniform field solution in a structure of permanent magnets.

[0064]FIG. 2 shows the basic schematic of a self-shielding structure of electric currents that generates a uniform field. {right arrow over (H)}_(h), {right arrow over (H)}_(h+1) are the intensities in the two regions that interface with the magnet cavity through boundaries S_(h), S_(h+1). Any combination of vectors {right arrow over (H)}_(h), {right arrow over (H)}_(h+1) whose tips belong to the dashed lines t_(h), t_(h+1) parallel to the interfaces, as shown in FIG. 1 is consistent with the existence of a uniform field solution. The orientation of vector {right arrow over (H)}_(h)−{right arrow over (H)}_(h+1) determines the orientation of interface, V_(h) and the magnitude of {right arrow over (H)}_(h)−{right arrow over (H)}_(H+1) determines the magnitude of the current density at V_(h). Intensities {right arrow over (H)}_(h), {right arrow over (H)}_(h+1) can be confined within the plane boundaries u_(h), u_(h+1) parallel to the intensities as shown in FIG. 2, if the current densities on u_(h), u_(h+1) are

{right arrow over (j_(1,h))} =−{right arrow over (η)}×{right arrow over (H)} _(h) , {right arrow over (j_(1,h)+1)} =−{right arrow over (η)}×{right arrow over (H)} _(h+1)   (2.1)

[0065] where unit vectors {right arrow over (η)} are perpendicular to u_(h), u_(h+1) and oriented outward with respect to the structure. By virtue of equations (2.1) the field vanishes in the external medium and is uniform in each region of the structure.

[0066] The current density on each interface can be generated by independent sources. The solution adopted according to the invention is based on dividing the structure in independent windings around each region V_(h), where the field has an intensity {right arrow over (H)}_(h), as shown in FIG. 3.

[0067] The current density {right arrow over (j)}_(h) on each face of Vh identified by subindex k is

{right arrow over (j)} _(h,k) =−{right arrow over (η)} _(h,k) ×{right arrow over (H)} _(h)   (2.2)

[0068] where unit vector {right arrow over (η)}_(h,k) is perpendicular to the k-th face and oriented outward with respect to V_(h).

[0069] The open magnet according to the invention is based on a closed structure of electric currents whose schematic is shown in FIGS. 4 and 5. It is a ring configuration with a winding V_(o) of circular cross-section of radius r₀ and three windings V₁, V₂, V₃ of elliptical cross-section whose major axis, equal to r₀, is oriented along the axis z. FIG. 4 shows an overall view of the structure and FIG. 5 shows its cross-section in the plane of symmetry z=0. The winding V_(o) is an open solenoid as shown in FIG. 6. The surface current density {right arrow over (j)}₀ is uniform and oriented perpendicular to y. Its magnitude is j₀=H₀.

[0070] The three windings V₁, V₂, V₃ are closed and carry uniform current densities $\begin{matrix} {j_{1} = {j_{2} = {j_{3} = \frac{j_{0}}{\cos \quad \alpha}}}} & (2.3) \end{matrix}$

[0071] where α is the angle between the axis of winding V₁ relative to the axis y, as shown in FIG. 5. The view of V₃ is presented in FIG. 6 which shows the electric current distribution on the interface between V₃ and V₁.

[0072] Winding V_(o) is assumed to enclose the region of interest of the magnet where the imaging is performed. By virtue of equation (2.3), the selection of the angle α≠0 results in a smaller cross-sectional area of V₁, V₂, V₃ compared to V_(o) and as a consequence, it results in a reduction of the magnet dimensions. The field uniformity is maintained as long as the magnet of FIG. 4 is a closed structure. Obviously, the winding V_(o) must be open in order to provide access to the region of interest. In a first approximation, the winding V_(o) is omitted.

[0073] A distortion of the field results from the opening, as well known in the art. The field distortion in the region of interest must be partially compensated in order to achieve the desired degree of uniformity within the imaging region. This can be accomplished by means of electric currents surrounding the opening of V_(o), designed to compensate for the lower order harmonics of the field distortion. The technique according the invention and defined in the following, involves the use of a filter structure composed of ferromagnetic materials and permanent magnets.

[0074] The schematic of FIG. 7 shows an ideal plane plate of infinite magnetic permeability and zero thickness inserted in a solenoid of infinite length in a plane perpendicular to the axis of the solenoid.

[0075] The plate extends arbitrarily in the external medium where the field is zero. Because the plate is perpendicular to the field generated by the solenoid, its insertion does not affect the field. In practice, the plate consists of a ferromagnetic medium of high magnetic permeability and finite thickness. As long as the ferromagnetic medium does not saturate at the field level generated by the current, the effect of its insertion in the solenoid can be computed as a linear problem where the plate acquires a given potential induced by the current.

[0076] Based on these considerations, the magnetic structure is opened by replacing the winding V_(o) of FIG. 4 with the pair of ferromagnetic plates located at the interfaces of windings V₁, V₃ as indicated in the schematic of FIG. 8 that is the basis for the design of the pole pieces of the magnet. The plates are assumed to be coaxial with the axis y, circular with a radius r_(e) equal or larger than the radius r₀ of the original winding V_(o) and at a distance 2y_(o) from each other. Because of symmetry, ±Φ_(o) are the values of the magnetostatic potential induced by the magnet on the two plates. The field configuration between the plates is illustrated by the equipotential lines shown in FIG. 9, computed on the assumption of infinite magnetic permeability μ. Because the two μ=∞ plates act as perfect magnetic mirrors, the magnetostatic potential Φ (r, ψ, y) generated between the plates, within a cylinder of radius r₁<r_(e) can be expanded in the series of cylindrical harmonics $\begin{matrix} {{\Phi \left( {r,\psi,y} \right)} = {{\Phi_{0}\frac{y}{y_{0}}} + {\Sigma \quad {{I_{m}\left( {n\quad \pi \frac{r}{y_{0}}} \right)}\left\lbrack {{a_{m,n,1}\cos \quad m\quad \psi} + {a_{m,n,2}\sin \quad m\quad \psi}} \right\rbrack}\sin \quad m\quad \pi \frac{y}{y_{0}}}}} & \text{(3.1)} \end{matrix}$

[0077] where Im is a modified Bessel function of the third kind. The terms of the sum are spatial harmonics of the field distortion caused by the finite radial dimensions of the plates. The terms m±0 are the harmonics resulting from the geometry of the windings of the structure, as well as the tolerances of materials and magnetic fabrication. As long as the radial dimensions of the plates are large compared to the gap 2y_(o), the magnitude of the of harmonics decreases rapidly with increasing values of m,n and the distortion is basically limited to lower order harmonics.

[0078] The elimination of the significant harmonics of the field distortion is accomplished by means of a structure attached to the ferromagnetic plates that acts as a spatial filter, following a technique developed by one of the inventors in recent years. The design of the filter is based on a modulation {overscore (Φ)} of the potential of the plates outside the cylinder of radius r₁ that is defining the radial extent of the relevant region, i.e., the imaging region. The distribution of the modulation {overscore (Φ)} is provided by the solution of the system of equations $\begin{matrix} {{\frac{\pi}{y_{0}^{2}}\left( {- 1} \right)^{n}n{\int_{0}^{2\pi}\quad {{\psi}{\int_{r_{i}}^{r_{e}}{{{rK}_{m}\left( {n\quad \pi \frac{r}{y_{0}}} \right)}{\Phi \left( {r,\psi} \right)}\begin{pmatrix} {\cos \quad m\quad \psi} \\ {\sin \quad m\quad \psi} \end{pmatrix}{r}}}}}} = \left( a_{m,n} \right)_{\begin{matrix} 1 \\ 2 \end{matrix}}} & (3.2) \end{matrix}$

[0079] where Km is a modified Bessel function of the third kind. A solution of system (3.2), applicable to the lower order harmonics, is obtained by dividing the area of the plates between r_(i) and r_(e) in a series of n_(o) concentric rings each composed of a number m_(o) of angular sectors, where each sector has a uniform value {overscore (Φ)}_(h,k) of the potential modulation {overscore (+101)}. The optimization of the ring structure results in the selection of a radial dimension Δ rh of the h-th ring $\begin{matrix} {{\Delta \quad r_{h}} = {\frac{y_{0}}{h\quad \pi}\quad \left( {{h = 1},2,3,\ldots} \right)}} & (3.3) \end{matrix}$

[0080] where the rings are numbered starting from the outermost ring of external radius r_(e). The modulation {overscore (Φ)}_(h,k) of the potential assumes a surface of distribution of dipole moments on the surface of the plates, with a dipole moment per unit surface {right arrow over (p)}_(h,k) in each sector equal to

{right arrow over (p)}_(h,k)=μ₀{overscore (Φ)}_(h,k){right arrow over (η)}  (3.4)

[0081] where unit vector {right arrow over (η)} is oriented perpendicular to the plate, as indicated in FIG. 8.

[0082] The solution of Eqs. (3.2) results in the potential modulations {overscore (Φ)}_(h,k) oscillating from positive to negative values from one ring to another. As a consequence, the orientation of dipole moment {right arrow over (p)}_(h,k) oscillates from parallel to opposite the intensity {right arrow over (H)}₀ from one ring to another, starting with a parallel orientation in the outermost ring. The distribution of {right arrow over (p)}_(h,k) can be implemented with layers of permanently magnetized material of remanence {right arrow over (J)} and thickness y_(h,k). In this solution, the rings where {right arrow over (J)} is oriented opposite to {right arrow over (H)}₀ require the selection of a high intrinsic coercivity material, to avoid its demagnetization. The dipole, moments {right arrow over (p)}_(h,k) can also be implemented by virtue of the equivalence of magnetized materials and electric currents by transforming each sector of the filter structure into a loop carrying an electric current I_(h,k) of magnitude

p_(h,k)=μ₀I_(h,k)   (3.5)

[0083] as indicated in the schematic of FIG. 10.

[0084] As a third option, the solution of Eqs. 3.2 can be used to replace the ferromagnetic plates with passive pole pieces, by transforming equipotential surfaces generated by the filter structure between the plates onto the surfaces of high magnetic permeability materials.

[0085] The schematic of the superconducting magnet is presented in FIG. 11, which shows the magnet cross-section in the plane x,y. The heavy lines W ₁, W₂, W₃ represent the cross-section of the superconducting conductors that are supported by three structures V₁, V₂, V₃. The schematic of FIG. 11 corresponds to a selection of an angle α=30° defined in FIG. 5. Thus the basic geometry of FIG. 11 corresponds to a value of the field intensity in each winding equal to twice the value of the intensity H_(o) within the region of interest. The three windings are assumed to be wound in a single layer on V ₁, V₂, V₃ and are connected in series as indicated in the schematic of FIG. 12 where S represents the superconducting shunt.

[0086] Because of symmetry, the pitch of the windings is the same on the surfaces of V₁, V₂, V₃ that form the two plane interfaces between V₁, V₂ and V₂, V₃.

[0087] Assume circular conductors of radius rω. FIG. 13 shows the relative position of the layers of the superconductors, with the assumption that the loops of the conductors are tangent to each other on the external surfaces of V₁, V₂, and V₃.

[0088]FIG. 10 shows that the winding V_(o) of the schematic of FIG. 4 is replaced by the structure of the two ferromagnetic parallel plates that form the pole pieces of the magnet. The central part of each plate (r<r_(i)) is the reference plane surface that establishes the dimension 2y_(o) of the reference system of the expansion (3.1) of the cylindrical harmonics. The external part of each plate (r₁<r<r_(e)) is the filter structure designed to cancel the harmonics. Each of the three options mentioned, or a combination of them, can be selected to design the filter structure.

[0089] In principle the generation of the dipole moments {right arrow over (p)}_(h,k) by means of electric currents distributed on the surface of each plate can result in a minimum volume of the filter structure and this is particularly true for the outer ring that compensates for the dominant fundamental harmonic (n=1).

[0090] By virtue of the theorem of equivalence of magnetization of electric currents, the surface current density {right arrow over (j)} that replaces a surface dipole moment density {right arrow over (p)} is $\begin{matrix} {\overset{\rightarrow}{j} = {\frac{1}{\mu_{0}}{\nabla{\times \quad \overset{\rightarrow}{p}}}}} & (4.1) \end{matrix}$

[0091] where {right arrow over (j)}, oriented parallel to the plate surface, satisfies the condition of continuity

∇·{right arrow over (j)}=0   (4.2)

[0092] Eq (4.1) transforms into $\begin{matrix} {{\Delta \cdot \overset{\rightarrow}{j}} = {{- \frac{1}{\mu_{0}}}{\nabla^{2}p}\quad \overset{\rightarrow}{y}}} & (4.3) \end{matrix}$

[0093] p is a continuous function of position, oscillating between positive and negative values, with maxima and minima within the area r₁<r<r_(e), p cannot be an harmonic function and the lines of flow of {right arrow over (j)} may close upon themselves within the area of the filter structure. In a polar coordinate system (r, ψ, y), by virtue of (4.1), the components of {right arrow over (j)} are: $\begin{matrix} {{j_{r} = {\frac{1}{\mu_{0}r}\frac{\partial p}{\partial\psi}}},{j_{\psi} = {{- \frac{1}{\mu_{0}}}\frac{\partial p}{\partial r}}}} & (4.4) \end{matrix}$

[0094] The differential equation of the lines of flux of {right arrow over (j)} is $\begin{matrix} {{\frac{1}{r}\frac{r}{\psi}} = \frac{j_{r}}{j\quad \psi}} & (4.5) \end{matrix}$

[0095] i.e., by virtue of (4.4) one has $\begin{matrix} {{{\frac{\partial p}{\partial r}\frac{r}{\psi}} + \frac{\partial p}{\partial\psi}} = 0} & (4.6) \end{matrix}$

[0096] and the equation of the lines of flux of {right arrow over (j)} is

p(r,ψ)=const   (4.7)

[0097] In general, because the solution of the system of Eqs.3.2 is a periodic function of ψ, the continuous distribution of p(r,ψ) can be written in the form $\begin{matrix} {{p\left( {r,\psi} \right)} = {\underset{m}{\Sigma}{R_{m}(r)}^{\quad m\quad \psi}}} & (4.8) \end{matrix}$

[0098] and if p is an harmonic function, R_(m)(r) in Eq.(4.8) must be a solution of the equation $\begin{matrix} {{{r\frac{\quad}{r}\left( {r\frac{R_{m}}{r}} \right)} - {m^{2}R_{m}}} = 0} & (4.9) \end{matrix}$

[0099] i.e.,

R_(m)=C_(m)r^(±m)   (4.10)

[0100] in which case, for each value of m, the filter structure is limited to the cancellation of a single harmonic of an assigned order m. Assume for instance that the mth term of series (4.8) is $\begin{matrix} {{p_{m}\left( {r_{i},v} \right)} = {{C_{m}\left\lbrack {\left( \frac{r}{r_{i}} \right)^{m} - \left( \frac{r_{i}}{r} \right)^{m}} \right\rbrack}{\cos \left( {m\quad \psi} \right)}}} & (4.11) \end{matrix}$

[0101] where constant C_(m) is designed to cancel coefficient am,n in expansion (3.1). Constant C_(m) is given by $\begin{matrix} {{\frac{( - )^{n}}{\mu_{0}y_{0}}{{{\frac{r^{m + 1}}{r_{i}^{m}}{K_{m + 1}\left( {n\quad \pi \quad \frac{r}{y_{0}}} \right)}} - {\frac{r_{i}^{m}}{r^{m - 1}}{K_{m - 1}\left( {n\quad \pi \quad \frac{r}{y_{0}}} \right)}}}}_{r_{i}}^{r_{e}}C_{m}} = a_{m,n,1}} & (4.12) \end{matrix}$

[0102] An example of line of flow of {right arrow over (j)} is shown in FIG. 14 for m=2. The circle of radius r₁, where p2=0, is a line of flow of {right arrow over (j)}. In the particular case where m=0, no current flows within the region of the filter structure, and the uniform value of p in the structure is obtained with equal currents flowing in opposite directions in two loops concentric with the center of the plate, as the boundaries of the r₁<r<r_(e) region.

[0103]FIG. 15 shows the lines of flux of {right arrow over (j)} as an example of a nonharmonic function $\begin{matrix} {{p\left( {r,\psi} \right)} = {{C_{m}\left\lbrack {i - {4\left( \frac{r - r_{c}}{r_{e} - r_{i}} \right)^{2}}} \right\rbrack}\cos \quad m\quad \psi}} & (4.14) \end{matrix}$

[0104] in the particular case m=2. r_(c) in Eq. (4.14) is $\begin{matrix} {r_{c} = {\frac{1}{2}\left( {r_{e} - r_{i}} \right)}} & (4.15) \end{matrix}$

[0105] The radial boundaries r=r₁, r=r_(e) of the filter structure are lines of flux of the current density that close upon themselves with the angular interval ψ=±π/4.

[0106] Another example of practical interest is the distribution of p independent of the radial coordinate

p(ψ)=C_(m) cos m ψ  (4.16)

[0107] which results in the surface current density $\begin{matrix} {{J_{r} = {{- \frac{{mC}_{m}}{\mu_{0}r}}\sin \quad m\quad \psi}},\begin{matrix} \quad & \quad & {J_{\psi} = 0} \end{matrix}} & (4.17) \end{matrix}$

[0108] As shown in FIG. 16, the radial lines of flux of {right arrow over (j)} close outside the r₁<r<r_(e) region.

[0109] The correction of the higher order harmonics of the field distortion involved the cancellation of small values of {overscore (101 _(h,k))}

|{overscore (Φ)}_(h,k)|<<Φ_(o)   (4.18)

[0110] In this case the h,k filter component can be reduced to a small dipole implemented by a cylinder of magnetized material located at the center of each filter sector, with a dipole moment

M_(h k)˜p_(h,k)S_(h,k)   (4.19)

[0111] where S_(h k) is the area of the sector. The cylinder of magnetized material can be replaced by a circular coil as shown in FIG. 17 of radial dimensions r₁, r₂ and height z₁ carrying a uniform current density i, with a dipole moment $\begin{matrix} {M_{h,k} = {\mu_{0}\frac{\pi \quad I_{h,k}}{3}\left( {r_{1}^{2} + r_{2}^{2} + {r_{1}r_{2}}} \right)}} & (4.20) \end{matrix}$

[0112] where

I_(h,k)=(r₂−r₁)₁i_(h,k)   (4.21)

[0113] The distribution of the equivalent dipole moment density generated by the coil is shown in FIG. 17.

[0114] The schematic of the pole pieces is shown in FIG. 17. The thickness of the plates is chosen to ensure the mechanical rigidity of the plates, particularly in the central region r<r₁ where the precision of the plate geometry and their relative position is most critical for achieving a high degree of field uniformity. As shown in FIG. 17, the external radius r_(c) of the plates is larger than r₀. The effect of r_(c)>r₀ is an increase in the degree of uniformity within the imaging region r<r₁ as shown in FIG. 18 where the component B_(y) is plotted vs. the axis y for several values of the plate overhang r_(e)-r₀. The uniformity improvement is achieved at the cost of a reduction of the volume of the field within the region of imaging. Obviously in the limit r_(e)→∞, the asymptotic value of the field intensity between the plates vanishes.

[0115] Although only preferred embodiments are specifically illustrated and described herein, it will be appreciated that many modifications and variations of the present invention are possible in light of the above teachings and within the purview of the appended claims without departing from the spirit and intended scope of the invention. 

1. A superconducting magnet, comprising: a region of interest in which a static magnetic field is generated, wherein a part under examination is placed for imaging, means for generating a uniform annular distribution of electric currents enclosing a polyhedral cavity.
 2. The superconducting magnet according to claim 1, wherein in that the distribution of electric currents is composed of uniform surface currents on interfaces towards the enclosed cavity, and on opposed plane peripheral boundaries surfaces; and in which the current density at each peripheral boundary surface is defined by {right arrow over (j_(1,h))} =−{right arrow over (η)}×{right arrow over (H)} _(h) where {right arrow over (η)} is a unity vector perpendicular to the corresponding peripheral plane boundary and {right arrow over (H)}_(h) is the intensity vector associated with the region enclosed by the plane boundary.
 3. The superconducting magnet according to claim 1, wherein in that the structure of currents may be divided into different regions each one having a correspondent interface to the polyhedral cavity and a correspondent peripheral boundary surface towards an external medium and each one having an adjacent region and a common plane interface to that adjacent region, except at the relevant which correspond to one of the said region in which the structure of currents is divided and at which the opening of the structure is provided where the said common plane interfaces of the end regions forms the two opposite surfaces delimiting the relevant region the current at the peripheral boundary of each region being defined by {right arrow over (j_(1,h))} =−{right arrow over (η)}×{right arrow over (H)} _(h) Where n is a unity vector perpendicular to the external plane boundary of the h-region and oriented outwards with reference to the centre of the cavity; Hh is the field intensity at the h-region.
 4. The superconducting magnet according to claim 1, wherein in that any combination of intensity vectors Hh, Hh+1 of the different regions of the current structure, for which the tips of the intensity vectors lay on ideal lines parallel to the corresponding interfaces to the cavity, the origin being defined by the common intersection axis of two adjacent or subsequent interfaces of adjacent or subsequent regions of the opened annular structure of currents may be used.
 5. The superconducting magnet according to claim 1, wherein the orientation of the difference vector of the magnetic intensity vectors of two adjacent or subsequent regions defines the orientation of the common plane interface between two subsequent or adjacent regions.
 6. A magnetic structure wherein the magnitude of the difference vector defines the current density at the plane common interface between the regions.
 7. The magnet according to claim 6, wherein the peripheral plane boundaries of each region is parallel to the intensity vector of the field generated in the said region or by the same field generating element.
 8. The magnet according to claim 6, wherein the current density on each interface may be generated by independent sources corresponding to the different regions, the superconducting magnet being formed by several coils the winding of which enclose polyhedral volumes having shape corresponding to the geometrical shape of the different region in which the structure of current is divided extending over the surfaces of the said volumes. the current density on each face of the winding being defined by, {right arrow over (j)} _(h,k) =−{right arrow over (η)} _(h,k)×{right arrow over (H)}_(h) where index h defines the different volumes of the different regions and k the different faces of the ideal geometric figure defining the said volume.
 9. The magnet according to claim 1, wherein the magnet has a closed annular shape enclosing a polyhedral cavity which forms the relevant region for carrying out imaging.
 10. The magnet according to claim 1, wherein the magnet is an open superconducting magnet which has means for generating a uniform annular distribution of electric currents enclosing the polyhedral cavity and in which the said distribution of currents being defined according to a correspondent closed distribution of currents according to one or more of the preceding claims 1 to 8 which distribution is opened at the relevant region for carrying out imaging.
 11. An open magnet according to claim 1, wherein that it has a ring configuration and is formed of three independent windings of elliptic form two of which has opposed parallel surfaces defining an opening of the ring configuration which corresponds to a fourth winding having circular cross section, the major axis of the two opposed elliptic windigs being equal one to the other and equal to the lacking circular winding.
 12. The open magnet according to claim 11, in which four winding are provided the one having circular cross-section being at least partially opened.
 13. The open magnet according to claim 11, wherein the magnet structure is a combination of superconducting windings and permanent magnets and/or ferromagnetic materials.
 14. The open magnet according to claim 13, wherein at the opening of the ring structure a filter structure is provided for compensating the low order harmonic magnetic filed distorsion at the relevant region where imaging has to be carried out by providing at the opposed and spaced apart interface surfaces defining the opening of the cavity plates of ferromagnetic materials and/or permanent magnets.
 15. The open magnet according to claim 13, wherein at the interfaces of the two opposite elliptic windings defining the opening of the magnet ferromagnetic plates are provided on each interface, each of the said ferromagnetic plates carries filter element which modulates the potential of the filed outside the region of interest, i.e. where imaging has to be carried out.
 16. The open magnet structure according to claim 15, wherein the filter structure is formed by one or more of concentric rings each of the said ring being formed by one or more sectors and each of the said sectors having a predetermined uniform value modulation of the magnetic potential.
 17. The open magnet according to claim 16, wherein the rings forming the filter structure are provided outside the relevant region, i.e. the region where imaging has to be performed.
 18. The open magnet according to claim 13, wherein the means for modulating the magnetic potential at the ferromagnetic plates are permanent magnetized dipoles.
 19. The open magnet according to claim 13, wherein the means for modulating the magnetic potential at the ferromagnetic plates are dipoles generated by electric currents.
 20. The open magnet according to claim 13, wherein the filter comprises means for correcting also distorsions of high order, the means being formed by cylinder or rings of magnetized material or equivalent electric current distriburtions each of which is associated to a magnetic dipole of one angular sector.
 21. The open magnet according to claim 13, wherein the filter structure is formed by ferromagnetic elements.
 22. The open magnet according to claim 13, wherein the filter structure is formed by a combination of ferromagnetic elements and magnetic dipoles generated either by permanent magnets or by electric currents.
 23. A method of using a superconducting magnet, comprising: generating a uniform annular distribution of electric currents enclosing a polyhedral cavity; and placing a part to be examined in a region of interest in which a static magnetic field is generated. 